三种基于2，4，6-三(3-吡啶基)-1，3，5-苯配体的Ni(Ⅱ)基配位聚合物的合成、结构及催化性能

通过调变溶剂热的反应条件,我们合成了3种Ni (Ⅱ)基的配位聚合物(CPs)[Ni (CH₃-BDC)(3-TBT)(H₂O)₂]·EtOH·2H₂O (CP1)、[Ni₃(CH₃-BDC)₃(3-TBT)₂(H₂O)₅]·2DMF·2H₂O (CP2)和[Ni₃(CH₃-BDC)₃(3-TBT)₂(H₂O)₆]·2DMF·4H₂O (CP3),其中CH₃-H₂BDC=5-methylisophthalic acid,3-TBT=2,4,6-tris (3-pyridyl)-1,3,5-benzene。X射线单晶衍射分析表明,3个CPs都是由相似的Ni₂(CH₃-BDC)₂的双核单元构建的,并分别呈现出从零维(0D)、2D到3D结构的网络骨架。反应条件的微小调变,导致了不同结构的配位聚合物。同时,催化实验表明,3在无溶剂的温和反应条件下,CP3对苄醇及其衍生物与苯胺的氧化-偶联反应表现出极好的催化活性和循环稳定性。     

氯化铜的少溶剂固态连串配位化学反应

在少量水的存在下,由于 NH₄[CuCl₃]对水不稳定,CuCl₂·2H₂O 与氯化铵的配位化学反应只能得到 1:2 产物(NH₄)₂[CuCl₄(H₂O)₂];但在无水乙醇中,无水 CuCl₂与氯化铵按 1:1或 1:2的物质的量之比混合时,能相应地得到 NH₄[CuCl₃]或(NH₄)₂[CuCl₄]。CuCl₂·2H₂O与 2,2''-联吡啶(bipy)的少溶剂固态化学反应仍能像固态化学反应一样,根据反应物的配比生成相应的唯一产物,但在物质的量之比为1:1的反应中发现1:2产物曾经形成。热力学分析说明,如果连串反应的后一步的Δ_rG^⊖大于前一步的,则上述反应现象是可能的。     

层状多硫代锑(Ⅲ)酸镉(Ⅱ)化合物(1,4-DABH2)Cd2Sb2S6的溶剂热合成与表征

利用溶剂热方法合成了层状多硫代锑髥酸镉髤化合物(1,4-DABH2)Cd2Sb2S6(1)(1,4-DAB=1,4-丁二胺),并通过红外光谱、热重分析对其进行了表征,用X-射线衍射测定了化合物的单晶结构。单晶解析表明,化合物属正交晶系,Cmca空间群,Mr=750.77,a=0.860 3(5)nm,b=0.898 7(6)nm,c=2.273(2)nm,V=1.758(2)nm3,Z=4,λ=0.071 073 nm,R=0.032,wR=0.106 7。晶体结构中含有六元环的Cd2SbS3和八元环的Cd2Sb2S4的阴离子网络层状[CdSbS3]nn-,双质子化的有机阳离子在阴离子层之间以氢键N-H…S形式连接。另外紫外-可见漫反射光谱研究表明,化合物为半导体。     

纳米镍钴铁氧体空心微球的制备与性能

以乙二醇为溶剂,氯化铁、氯化钴、氯化镍和醋酸铵为反应试剂,采用溶剂热法制备纳米Ni_xCo_1-xFe₂O₄(x=0、0.3、0.5、0.7、1)铁氧体空心微球,研究镍含量对铁氧体空心球的磁性与吸波性能的影响。借助X-射线衍射仪(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、振动样品磁强计(VSM)和网络分析仪对试样的物相组成、微观形貌和电磁特性进行表征。结果表明制备的镍钴铁氧体为尖晶石结构,且形貌为空心球,粒径在200 nm左右。当x=0时,镍钴铁氧体空心球饱和磁化强度最大为81.7 emu·g^-1,反射损耗在1 658.8 MHz有最小值为-16.9 dB。     

溶剂热法制备立方状ITO粉体及其电性能

以乙二醇、乙醇为溶剂通过溶剂热法制备出立方状ITO纳米粉体,研究了反应时间、NaOH浓度对ITO纳米粉体形貌的影响,并讨论了溶剂体积比、NaOH浓度对ITO粉体导电性的影响及机理。结果表明：采用乙二醇与乙醇做溶剂,V_EG：V_EtOH=4：1时,制备出分散性良好的立方状ITO纳米粉体,平均粒径为10.7 nm,且其XRD衍射峰强度比I₄₀₀/I₂₂₂最高为0.380;乙二醇与乙醇做溶剂,V_EG：V_EtOH=4：1,且NaOH浓度为0.275 mol·L^-1时,粉体电导率最高为46.75 mS·cm^-1。     

硫辛酸抗氧化性溶剂效应的理论研究

采用密度泛函方法,利用自洽反应场(SCRF)的Onsager模型,研究了正庚烷、苯、二氯甲烷、乙醇、二甲亚砜和水六种不同溶剂中硫辛酸分子的抗氧化性。以S-S键键解离焓(BDE)和分子电离势(IP)为理论指标评价了硫辛酸在六种溶剂中清除自由基的活性。发现随着溶剂的介电常数增大,BDE值几乎不变,而IP值则显著减小,表明溶剂效应对清除自由基的电子转移反应机理影响更大。溶剂的极性较小时,偏向于形成硫自由基的机理,而溶剂的极性较大时,偏向于电子转移机理。     

顶空气相色谱法测定瑞替加滨原料药中残留溶剂

建立了测定瑞替加滨原料药中残留溶剂乙醇、正己烷、四氢呋喃、三乙胺的顶空气相色谱方法。采用氢火焰离子化检测器,以N,N-二甲基甲酰胺为样品溶剂,通过对色谱条件优化,建立了以DB-624为分析柱、110℃为平衡温度、15 min为平衡时间的残留溶剂测定方法。经方法学验证,上述4种溶剂的方法检出限依次为0.007 5%、0.000 48%、0.002 4%、0.01%;峰面积的相对标准偏差均小于2.1%;平均回收率为100%～102%;4种溶剂的线性系数均大于0.995。结果表明,该方法的检测灵敏度高、精密度好、准确度高、线性关系良好,能够满足对瑞替加滨质量的控制要求。将该方法应用于3批瑞替加滨原料药的残留溶剂检测,均只检出乙醇和正己烷,且乙醇和正己烷的最高残留量分别为0.149%和0.022%,均未超出限量规定。     

Ion Pairing Kinetics Does not Necessarily Follow the Eigen-Tamm Mechanism

The most recognized and employed model of the solvation equilibration in the ionic solutions was proposed by Eigen and Tamm, in which there are four major states for an ion pair in the solution： the completely solvated state, 2SIP （double solvent separate ion pair）, SIP （single solvent separate ion pair）, and CIP （contact ion pair）. Eigen and Tamm suggested that the transition from SIP to CIP is always the slowest step during the whole pairing process, due to a high free energy barrier between these two states. We carried out a series of potential of mean force calculations to study the pairing free energy profiles of two sets of model mono- atomic 1：1 ion pairs 2.0：x and x：2.0. For 2.0：x pairs the free energy barrier between the SIP and CIP states is largely reduced due to the salvation shell water structure. For these pairs the SIP to CIP transition is thus not the slowest step in the ion pair formation course. This is a deviation from the Eigen-Tamm model.     

Theoretical Insights into Intermolecular Hydrogen-Bonding Strengthening in Fluorenone-Methanol Complexes Induced by Electronic Excitation and Bulk Solvent Effect

This work presents a theoretical insight into the variation of the site-specific intermolecular hydrogen-bonding （HB）, formed between C=O group of fluorenone （FN） and O-H groups of methanol （MeOL） molecules, induced by both the electronic excitation and the bulk solvent effect. Through the calculation of molecular ground- and excited-state properties, we not only demonstrate the characters of HB strengthening induced by electronic excitation and the bulk solvent effect but also reveal the underlying physical mechanism which leads to the HB variation. The strengthening of the intermolecular HB in electronically excited states and in liquid solution is characterized by the reduced HB bond-lengths and the red-shift IR spectra accompanied by the increasing intensities of IR absorption corresponding to the characteristic vibrational modes of the O-H and C--O stretching. The HB strengthening in the excited electronic states and in solution mainly arises from the charge redistribution of the FN molecule induced by the electronic excitation and bulk solvent instead of the intermolecular charge transfer. The charge redistribution of the solute molecule increases the partial dipole moment of FN molecule and the FN-MeOL intermolecular interaction, which subsequently leads to the HB strengthening. With the bulk solvent effect getting involved, the theoretical IR spectra of HBed FN-MeOL complexes agree much better with the experiments than those of gas-phase FN-MeOL dimer. All the calculations are carried out based on our developed analytical approaches for the first and second energy derivatives of excited electronic state within the time-dependent density functional theory.     

A New Coordination Polymer Containing 4-[（8-Hydroxy-5-quinolinyl）azo]-benzenesulfonic Acid： Synthesis,Structure and Fluorescent Property

A new coordination polymer, {[CdL（en）]＇DMF}n （1, H2L = 4-[（8-hydroxy-5- quinolinyl）azo]-benzenesulfonic acid, en = ethylenediamine, DMF = N,N-dimethylformamide）, has been solvothermally synthesized and structurally characterized by single-crystal X-ray diffrac- tion, infrared （IR） spectra, elemental analysis, powder X-ray diffractions （PXRD） and thermo- gravimetric analysis （TGA）. Compound 1 crystallizes in monoclinic, space group P2Jc with a = 14.6525（9）, b = 13.3917（9）, c = 11.8838（8） A, β = 101.2290（10）°, V = 2287.2（3） A3, Z = 4, C20H24CdN6OsS, Mr = 572.91, Dc. = 1.664 mg-mm-3, F（000） = 1160, p = 1.091 mm-1, R = 0.0232 and wR = 0.0587 for 3597 observed reflections （I 〉 2σ（I））. Compound 1 exhibits a one-dimensional （1D） double-chain structure which is further connected through hydrogen bonding and π-π interactions into a three-dimensional （3D） supramolecular network. In addition, it exhibits blue fluorescence at room temperature in the solid state.